TECHNICAL FIELD
[0001] The present invention relates generally to high-voltage field effect transistors
(FETs); more specifically, to high-electron-mobility transistors (HEMTs) and heterostructure
field-effect transistors (HFETs), and to methods of fabricating such power transistor
devices.
BACKGROUND
[0002] One type of high-voltage FET is a heterostructure FET (HFET), also referred to as
a high-electron mobility transistor (HEMT). HFETs based on gallium nitride (GaN) and
other wide bandgap nitride III based direct transitional semiconductor materials,
such as silicon carbide (SiC), are advantageously utilized in certain electronic devices
due to their superior physical properties over silicon-based devices. For example,
GaN and AlGaN/GaN transistors are commonly used in high-speed switching and high-power
applications (e.g., power switches and power converters) due to the high electron
mobility, high breakdown voltage, and high saturation electron velocity characteristics
offered by GaN-based materials and device structures. Due to the HFETs physical properties,
HFETs may change states substantially faster than other semiconductor switches that
conduct the same currents at the same voltages and the wide bandgap may improve performance
of the HFET at elevated temperatures.
[0003] GaN-based HFETs devices typically include a gate member formed over a thin gate dielectric
(e.g., oxide) material. In the past, interface states between the gate oxide and underlying
GaN layers have played a major role in the stability and electrical reliability of
GaN-based HFETs. Improving the gate stability is necessary to achieve high voltage
operations (e.g., 600 V). Typical prior art HFET gate structures include Schottky
gates, which have no gate oxide, or a single, thin gate oxide layer. These structures
suffer from low critical voltage usually in the range of 20-40 V. The critical voltage,
V
CRIT, is defined as the gate-to-source voltage, V
GS, at which there is a relatively sharp rise in the gate leakage current.
[0004] Properties of the gate dielectric also affect other parameters and characteristics
of the HFET. For example, the thickness of the gate dielectric layer plus the thickness
of the underlying barrier layer partially determine the gate threshold voltage of
a high-voltage HFET. Whereas a thicker gate dielectric reduces gate leakage current
with increased temperature or increased applied gate voltage, the thickness of the
gate dielectric contributes to the threshold voltage. As such, a trade-off exists
between thermal and voltage stability versus the ability to provide a constant threshold
voltage for the HFET device.
BRIEF DESCRIPTION OF THE DRAWINGS
[0005] Non-limiting and non-exhaustive embodiments of the present invention are described
with reference to the following figures, wherein like reference numerals refer to
like parts throughout the various views unless otherwise specified.
[0006] FIG. 1 is a cross-sectional side view of an example semiconductor device having a multiple-layer,
gate dielectric structure.
[0007] FIG. 2 is a diagram illustrating an example process flow for fabricating a semiconductor
device having a multiple-layer, gate dielectric structure.
[0008] FIG. 3 is a diagram illustrating another example process flow for fabricating a semiconductor
device having a multiple-layer, gate dielectric structure.
[0009] FIG. 4 is a graph illustrating example gate leakage increases versus applied gate voltage
for various semiconductor devices.
[0010] Corresponding reference characters indicate corresponding components throughout the
several views of the drawings. Skilled artisans will appreciate that elements in the
figures are illustrated for simplicity and clarity and have not necessarily been drawn
to scale. For example, the dimensions of some of the elements in the figures may be
exaggerated relative to other elements to help to improve understanding of various
embodiments of the present invention. Also, common but well-understood elements that
are useful or necessary in a commercially feasible embodiment are often not depicted
in order to facilitate a less obstructed view of these various embodiments of the
present invention.
DETAILED DESCRIPTION
[0011] In the following description, numerous specific details are set forth in order to
provide a thorough understanding of the present invention. It will be apparent, however,
to one having ordinary skill in the art that the specific detail need not be employed
to practice the present invention. In other instances, well-known materials or methods
have not been described in detail in order to avoid obscuring the present invention.
[0012] Reference throughout this specification to "one embodiment", "an embodiment", "one
example" or "an example" means that a particular feature, structure or characteristic
described in connection with the embodiment or example is included in at least one
embodiment of the present invention. Thus, appearances of the phrases "in one embodiment",
"in an embodiment", "one example" or "an example" in various places throughout this
specification are not necessarily all referring to the same embodiment or example.
Furthermore, the particular features, structures or characteristics may be combined
in any suitable combinations and/or sub-combinations in one or more embodiments or
examples. Particular features, structures or characteristics may be included in an
integrated circuit, an electronic circuit, a combinational logic circuit, or other
suitable components that provide the described functionality. In addition, it is appreciated
that the figures provided herewith are for explanation purposes to persons ordinarily
skilled in the art and that the drawings are not necessarily drawn to scale.
[0013] As used herein, the "critical voltage" or "critical gate voltage" of a HFET device
is defined as the gate-to-source voltage at which there is a relatively sharp rise
in the gate leakage current. Thermal stability relates to how much the gate leakage
current of the device increases with temperature.
[0014] As mentioned above, typical HFET gate structures include Schottky gates, which have
no gate oxide, or a single, thin gate oxide layer. These structures suffer from low
critical voltage usually in the range of 20-40 V. The critical voltage, V
CRIT, is defined as the gate-to-source voltage, V
GS, at which there is a relatively sharp rise in the gate leakage current. To achieve
high reliability and high gate oxide integrity, the critical voltage needs to be increased
from the present range of 20-40 V. Further, devices with a single, thin gate oxide
layer may experience an increase in gate leakage current two or three times larger
than the leakage current at room temperature when the device is operating at high
temperatures (such as 120 degrees Celsius).
[0015] In accordance with embodiments of the present invention, a GaN-based HFET device
and method of fabricating the same is disclosed which includes a multi-layer gate
dielectric structure. In one embodiment, the HFET device has first and second active
layers with a two-dimensional electron gas layer forming therebetween. A first gate
dielectric layer is disposed on the second active layer. Nitride-based compounds such
as silicon nitride (SiN), carbon nitride (CN) or boron nitride (BN) may be utilized
for first gate dielectric layer 108. A second gate dielectric layer is disposed on
the first gate dielectric layer. In one example, aluminum oxide (Al
2O
3) may be used for the second gate dielectric layer. A gate is disposed on the second
gate dielectric layer. Ohmic contacts (source and drain) of the device extend through
the first and second gate dielectric layers.
[0016] In various embodiments this multiple gate dielectric structure may result in very
high critical voltage operation (e.g., >80 V). Further, a device utilizing a multiple
gate dielectric structure may experience improved thermal stability. The device may
experience substantially no change in the leakage current when the device is operating
at temperatures upwards to 200 degrees Celsius. In addition to producing a more stable
and robust gate dielectric structure, other benefits observed include lower gate leakage
and a more uniform gate threshold voltage. The multi-layer gate dielectric structure
also allows the HFET device to maintain a constant threshold voltage while minimizing
gate leakage current.
[0017] In one embodiment, an Atomic Layer Deposition (ALD) reaction chamber technique is
utilized to form a thin layer of a nitride compound (e.g., SiN) in-situ over active
transistor device layers, immediately followed by a thin Al
2O
3 deposition by ALD. The term "in-situ" refers to a process that is carried out within
a single tool or reaction chamber without exposing the wafer to the environment outside
the tool or chamber. Further, the term "ex-situ" may refer to a process that is not
carried out in a single tool. First gate dielectric 108 may also be deposited using
metal-organic chemical vapor decomposition (MOCVD). Further, the first gate dielectric
108 may be deposited in-situ with the first and second active layers 102 and 106,
respectively. In another embodiment, first gate dielectric 108 may be deposited ex-situ
from the respective first and second active layers 102 and 106 through atomic layer
deposition (ALD). As configured in FIG. 1, the multi-layer gate dielectric structure
includes a Al
2O
3 layer disposed atop of a Si
3N
4 layer.
[0018] In the descriptions below, an example HFET is used for the purpose of explanation.
However, it should be appreciated that embodiments of the present invention may be
utilized with other types of FETs, such as a metal oxide semiconductor FET (MOSFET)
or metal insulator semiconductor FET (MISFET) devices.
[0019] FIG. 1 illustrates a cross-sectional side view of a semiconductor device 100 (e.g.,
a GaN HFET) which includes a first active layer 102, a second active layer 106, a
first gate dielectric 108, a second gate dielectric 110, a passivation layer 112,
ohmic contacts 116 and 118, and gate 114. Further shown in FIG. 1 is a layer of electrical
charge layer 104 which may form between the first active layer 102 and the second
active layer 106 due to the bandgap difference between the two layers. The layer of
electrical charge layer 104 defines the lateral conductive channel which is sometimes
called a two-dimensional electron gas (2DEG) layer 104 because electrons, trapped
in a quantum well that results from the bandgap difference between the first and second
active layer 102 and 106 are free to move in two dimensions but are tightly confined
in the third dimension. Further, the first active layer 102 is sometimes called a
channel layer while the second active layer 106 is sometimes called the barrier layer
or donor layer.
[0020] The second active layer 106 is disposed on first active layer 102. First gate dielectric
layer 108 is disposed on second active layer 106. A second gate dielectric layer 110
is disposed on first gate dielectric layer 108. A passivation layer 112 is disposed
on second gate dielectric layer 110. A gate 114 extends vertically down through passivation
layer 112 to second gate dielectric layer 110. Respective source and drain ohmic contacts
116 & 118 are shown extending vertically down through passivation layer 112, second
gate dielectric layer 110, and first gate dielectric layer 108 to electrically connect
to second active layer 106. As shown, source and drain ohmic contacts 116 & 118 are
laterally spaced-apart, with gate 114 being disposed between source and drain ohmic
contacts 116 & 118.
[0021] It is appreciated that first active layer 102 is typically disposed over a substrate
(not shown) formed of any one of a number of different materials, such as sapphire
(Al
2O
3), silicon (Si), GaN, or silicon carbide (SiC). In one embodiment, first active layer
102 comprises an epitaxial GaN layer. To avoid possible problems with lattice mismatch
and/or differences in thermal coefficients of expansion, one or more additional layers
may be disposed between the substrate and first active layer 102. For example, an
optional thin nucleation layer may be formed between the substrate and first active
layer 102. In other examples, first active layer 102 may comprise different semiconductor
materials containing nitride compounds of other Group III elements. The first active
layer 102 may be grown or deposited on the substrate.
[0022] In the example of FIG. 1 second active layer 106 comprises aluminum gallium nitride
(AlGaN). In other examples, different Group III nitride semiconductor materials such
as aluminum indium nitride (AlInN) and aluminum indium gallium nitride (AlInGaN) may
be used for second active layer 106. In other embodiments, the material of second
active layer 106 may be a non-stoichiometric compound. In such materials, the ratios
of the elements are not easily represented by ordinary whole numbers. For example,
the second active layer 106 may be a non-stoichiometric compound of a Group III nitride
semiconductor material such as Al
XGa
1-XN, where 0<X<1. The second active layer 106 may be grown or deposited on the first
active layer 102.
[0023] Also shown in FIG. 1 is a first gate dielectric layer 108 disposed on the second
active layer 106. In one embodiment, first gate dielectric layer 108 comprises silicon
nitride (SiN). In other embodiments, first gate dielectric layer 108 may comprise
Si
3N
4. In still other examples, different nitride-based compounds such as carbon nitride
(CN) or boron nitride (BN) may be utilized for first gate dielectric layer 108. The
first gate dielectric layer 108 may be a nitride based material which may conserve
the atomic arrangement with the second active layer 106. Further, the first gate dielectric
layer 108 may be insulating and have a band gap of at least 3 electron volts (eV).
In one example, the thickness of first gate dielectric layer 108 may be substantially
between 1-5 nanometers (nm) thick. First gate dielectric layer may be deposited in-situ
with first and second active layers 102 and layer 106, respectively. First gate dielectric
108 may be deposited using metal-organic chemical vapor decomposition (MOCVD). In
another embodiment, first gate dielectric 108 may be deposited ex-situ from first
and second active layers 102 & 106 through atomic layer deposition (ALD).
[0024] As shown, second gate dielectric layer 110 disposed on first gate dielectric layer
108. In one example, second gate dielectric layer 110 comprises aluminum oxide (Al
2O
3). In still further examples, other oxide materials, such as ZrO, HfO, SiO
2 and GdO, may be utilized for the second gate dielectric layer 110. In one embodiment,
second gate dielectric layer 110 has a thickness in the range of approximately 10-20
nm thick. In one embodiment, the second gate dielectric layer 110 is thicker than
the first gate dielectric layer 108. For example, the thickness of first gate dielectric
layer may be in a range of approximately 10-50 angstroms (A). In one example fabrication
process, second gate dielectric layer 110 may be deposited ex-situ from respective
first and second active layers 102 &106 utilizing atomic layer deposition (ALD).
[0025] Passivation layer 112 is disposed on second gate dielectric layer 110 and laterally
surrounds ohmic contacts 116, 118, and gate 114. In one embodiment, passivation layer
112 may comprise a dielectric material such as silicon nitride (SiN). In further embodiments,
passivation layer 112 may comprise multiple layers of material. Passivation layer
112 provides stability of the electrical characteristics of the device by isolating
the surface of the device from electrical and chemical contaminants of the environment.
Passivation layer 112 may be deposited through chemical vapor deposition such as low
pressure chemical vapor deposition (LPCVD) or plasma-enhanced chemical vapor deposition
(PECVD).
[0026] First and second gate dielectric layers 108 & 110 separate gate 114 from second active
layer 106. As shown, gate 114 is disposed through passivation layer 112 to contact
second gate dielectric layer 110. In one embodiment, gate 114 comprises a gold nickel
(NiAu) alloy. In another embodiment, gate 114 comprises a titanium gold (TiAu) alloy
or molybdenum gold MoAu alloy. In other examples, gate 114 may comprise a gate electrode
and gate field plate. In operation, gate 114 controls the forward conduction path
between ohmic source and drain contacts 116 & 118. In an example fabrication process,
gate 114 may be formed by etching an opening in passivation layer 112, followed by
a gate metal deposition. In the example of FIG. 1, the portion of gate 114 which is
above passivation layer 112 and extends laterally towards ohmic drain contact 118
serves as a gate field plate, which functions to alleviate the electric field intensity
at an edge (closest to ohmic contact 118).
[0027] Ohmic contacts 116 and 118 are disposed through passivation layer 112, second gate
dielectric layer 110, and first gate dielectric layer 108 to contact the second active
layer 106. Ohmic contact 116 is one example of a source contact, while ohmic contact
118 is one example of a drain contact. In one embodiment, ohmic contacts 116 and 118
may be formed by etching openings in passivation layer 112, second gate dielectric
layer 110, and first gate dielectric layer 108, followed by a metal deposition and
annealing steps. In another example fabrication process, ohmic contacts 116 and 118
may be formed before the deposition of second gate dielectric layer 110 and passivation
layer 112.
[0028] As shown, FIG. 1 illustrates the device structure at a point in the fabrication process
just after formation of ohmic metal contacts 116 and 118, which respectively comprise
source and drain electrodes of GaN HFET device 100. FIG. 1 shows ohmic metal contacts
116 and 118 formed directly on the second active layer 106. In other embodiments,
ohmic metal contacts 116 and 113 may be formed in recesses which extend vertically
downward into the second active layer 106. In other embodiments, ohmic metal contacts
116 and 118 may be formed in recesses that extend vertically downward through second
active layer 106 to contact the first active layer 102.
[0029] When HFET device 100 is configured for use as a power switch, gate 114 and ohmic
contacts 116 & 118 are typically coupled through terminals to form electrical connections
to external circuits. In operation, electric charge in 2DEG layer 104 flows laterally
between the ohmic contacts 116 and 118 to become a current in an external circuit.
The electric charge flow, and hence the current, may be controlled by a voltage from
an external circuit that is electrically connected between the gate 114 and ohmic
contact 116.
[0030] As used in this disclosure, an electrical connection is an ohmic connection. An ohmic
connection is one in which the relationship between the voltage and the current is
substantially linear and symmetric for both directions of the current. For example,
two metal patterns that contact each through only metal are electrically connected.
In contrast, ohmic contacts 116 and 118 are not electrically connected to each other
in HFET device 100 because any connection between these two contacts is through a
channel in the semiconductor material, which conduction path is controlled by gate
114. Similarly, gate 114 is not electrically connected to second active layer 106
since first and second gate dielectric layers 108 and 110 insulate gate 114 from the
underlying active layers.
[0031] In the embodiments described above, the thicknesses of the first and second gate
dielectric layers 108 and 110 are such that the gate leakage current remains substantially
constant over temperature during normal operation of HFET device 100. Stated differently,
HFET device 100 does not experience any substantial change in gate leakage current
when the device is operating at 120 °C. In addition, various embodiments of the present
invention may operate up to 200 °C without significant changes to the gate leakage
current.
[0032] Furthermore, the inventors have observed that the multiple gate dielectric layer
structure described herein improves the voltage stability of the HFET device. For
example, the critical voltage of HFET device 100 is significantly increased over prior
art device structures to range of approximately 100-130 V.
[0033] FIG. 2 is a diagram 200 illustrating an example process flow for fabricating a semiconductor
device such as HFET device 100 shown in FIG. 1. In the example shown, the process
starts after both the first and second active layer layers have been deposited or
grown on a substrate. To begin, a first gate dielectric layer comprising SiN is grown
in-situ (block 202). In one embodiment, the first gate dielectric layer is deposited
using a MOCVD technique carried out at a temperature range between 800-1050 °C. The
first gate dielectric layer is formed to a thickness of approximately 1-5 nm, and
is continuous over the surface of the wafer. In one embodiment, the thickness of the
gate dielectric layer is about 4 nm. In another embodiment, the first gate dielectric
layer is formed in-situ with the first and second active layers. For example, the
same machine (MOCVD) that is used to form the first and second active layers may also
be used to form the first gate dielectric layer. In other embodiments the first gate
dielectric layer may be deposited ex-situ from the first and second active layers.
[0034] Next, at block 204, the second gate dielectric layer is deposited atop the first
gate dielectric layer. In one embodiment, the second gate dielectric layer is deposited
on the wafer surface ex-situ from the first gate dielectric layer, and the first and
second active layers, at 300 °C using ALD. In one embodiment, the second gate dielectric
layer is deposited using ALD with an Al(CH
3)
3 precursor and O
2 plasma. The second gate dielectric layer is formed to a thickness in a range of approximately
10-20 nm. In a specific implementation, the second gate dielectric layer is about
15 nm thick.
[0035] In another embodiment, the first and second gate dielectric layers may be deposited
ex-situ from the first and second active layers. For example, both the first and second
gate dielectric layers may be deposited on the wafer surface using the same ALD chamber.
[0036] The process continues at block 206, at which point the second gate dielectric layer
undergoes high temperature annealing to improve the film and interface quality of
the second gate dielectric layer. By way of example, the annealing step may be performed
in a furnace at temperature range of 450-750 °C for approximately 5-10 minutes. Annealing
may also be performed using a number of different tools, such as a rapid temperature
annealing (RTA) tool.
[0037] After annealing, a passivation layer is deposited over the second gate dielectric
layer (block 208). In one embodiment, the passivation layer may be deposited using
PECVD. The passivation layer may also be deposited using LPCVD. The passivation layer
is typically formed to a thickness in a range of approximately 100-150 nm. As discussed
above, the passivation layer may comprise silicon nitride (SiN) or other materials
having similar properties.
[0038] At block 210, the surface of the passivation layer 112 undergoes mesa isolation etching
to define the active region of the ohmic contacts 116 and 118. In other words, mesa
isolation etching defines the footprint of the ohmic contacts 116 and 118. The mesa
isolation may be performed utilizing a reactive-ion etching (RIE) system. Further,
the mesa isolation may be performed using inductively coupled plasma (ICP) RIE.
[0039] Following mesa isolation, ohmic source and drain contacts are formed through the
passivation layer, second gate dielectric layer, and first gate dielectric layer (block
212). This involves first forming openings through the afore-mentioned layers, and
then depositing a metal or metal alloy to fill the openings. In one example fabrication
sequence, the metal utilized for the ohmic contacts is deposited using e-beam metal
evaporation. An example ohmic contact metal is TiAlMoAu. The metal ohmic contacts
are then annealed utilizing a RTA tool at a temperature range of approximately 600-900
°C (block 214).
[0040] The gate may be formed in a similar manner as the ohmic contacts. That is, the gate
may be formed by first etching an opening though passivation layer to expose the second
gate dielectric layer (block 216). In one embodiment, dry etching is performed utilizing
a gas such as CF
4 or SF
6. After the etching process exposes the second gate dielectric layer, a gate metal
or metal alloy deposition (block 218) is performed to fill the etched opening. In
one example, NiAu is used as the gate metal. As shown in FIG. 1, a field plate portion
may be formed by masking or etching the gate metal such that a top portion laterally
extends over the passivation layer towards the farthest (drain) ohmic contact.
[0041] Persons of ordinary skill in the semiconductor arts will understand that other standard
post-fabrication or back-end processing steps may be performed, including forming
metal (e.g., patterned lines or traces) on the surface of the wafer, wafer backgrinding
(also called backlapping or wafer thinning), die separation, and packaging.
[0042] FIG. 3 is a diagram 300 illustrating another example process flow for fabricating
a HFET semiconductor device having a multiple-layer, gate dielectric structure. Flow
diagram 300 is similar to flow diagram 200 except the process for forming the ohmic
contacts occurs prior to passivation.
[0043] The process begins after the first active layer and second active layer are deposited
or grown on a substrate. At block 302, the first gate dielectric layer is deposited
in-situ. The first gate dielectric layer may be deposited using MOCVD at a temperature
range between 800 to 1050 °C. The thickness of the first gate dielectric layer 108
is substantially between 1-5 nm and is continuous over the surface of the wafer. In
one embodiment, the thickness of the gate dielectric layer is 4 nm. However, similar
to mentioned above, the first gate dielectric layer may be deposited ex-situ from
the first and second active layers. Further, the first gate dielectric layer may be
deposited in the same machine as the second gate dielectric layer.
[0044] After growth of the first gate dielectric, the surface of the first gate dielectric
layer undergoes mesa isolation etching to define the active region of the ohmic contacts
(block 304). The mesa isolation may be performed utilizing a reactive-ion etching
(RIE) system. In other fabrication methods, the mesa isolation may be performed using
inductively coupled plasma (ICP) RIE. At this point in the process flow, ohmic via
openings may optionally be formed through the first gate dielectric layer, followed
by ohmic metallization and annealing at 850 °C for about one minute (block 306).
[0045] Next, the second gate dielectric layer is deposited on the first gate dielectric
layer (block 310). The second gate dielectric layer may also be deposited over the
source and drain ohmic contacts. In one embodiment, the second gate dielectric layer
is deposited on the wafer surface using ALD at 300 °C. The second gate dielectric
layer may be grown to a thickness of approximately 10-20 nm. In one embodiment, the
deposition of the second gate dielectric layer may be performed ex-situ from the first
and second active layers.
[0046] A high temperature anneal may be performed after the second gate dielectric layer
has been deposited (block 312). The temperature of the annealing may be between 500
to 700 °C and can be applied using either a furnace or a rapid temperature annealing
(RTA) tool. This annealing step improves the film and interface quality of the second
gate dielectric layer.
[0047] Following annealing a passivation layer is formed on the second gate dielectric layer
(block 314). In one embodiment, the passivation layer may be deposited using PECVD.
The passivation layer may also be deposited using LPCVD. The thickness of the passivation
layer may be between about 100-150 nm thick. As mentioned above, the passivation layer
may comprise silicon nitride (SiN).
[0048] Gate via formation is shown occurring next at block 316. This step is performed by
masking and then etching passivation layer such that an opening is formed through
the passivation layer, thereby exposing the second gate dielectric layer. In one embodiment,
dry etching may be utilized with a gas such as CF
4 or SF
6 to etch through the passivation layer. At block 318, the gate metal is deposited
in the gate via opening. In one example, NiAu is utilized as the gate metal. As shown
in FIG. 1, the gate member includes a field plate portion that extends toward the
drain ohmic contact. In one embodiment, the passivation layer and second gate dielectric
layer may undergo further etching and metal deposition to include field plate portions
for both ohmic contacts.
[0049] FIG. 4 is a graph illustrating example gate leakage increases versus applied gate
voltage for various HFET devices each having different gate dielectric structures.
As shown, the x-axis represents absolute gate voltage 404 while the y-axis is a ratio
of gate leakage increase 402. The ratio of the gate leakage current shown on y-axis
402 represents the ratio of the leakage current of the device under stress to the
leakage current of the device before stress. Graph 400 further shows a critical threshold
level 406. The critical threshold 406 may be defined as the threshold where the ratio
of gate leakage increase 402 is no longer acceptable and the device is considered
in breakdown. For the example shown, the critical threshold 406 is substantially 10.
In addition, the critical voltage refers to the gate voltage at which the ratio of
gate leakage increase for the particular device reaches the critical threshold 406.
[0050] As shown, graph 400 illustrates the performance of a first group of devices 408,
and a second group of devices 410. The gate voltage for each of the various groups
of devices is increased while the ratio of gate leakage increase 402 is measured.
For the first group of devices 408, the critical voltage is approximately 30-40 V.
For the second group of devices 410, the critical voltage is approximately 95-100
V. The first group of devices 410 represents devices with a single gate dielectric
layer (Al
2O
3) while the second group 410 represents devices with multiple gate dielectric layers.
As illustrated, the second group of devices 410 represents devices that each has a
first gate dielectric layer about 4 nm thick. As illustrated in FIG. 4, the critical
voltage may be substantially increased when multiple gate dielectric layers are utilized
in accordance with the embodiments of the present invention.
[0051] The above description of illustrated examples of the present invention, including
what is described in the Abstract, are not intended to be exhaustive or to be limitation
to the precise forms disclosed. While specific embodiments of, and examples for, the
invention are described herein for illustrative purposes, various equivalent modifications
are possible without departing from the broader spirit and scope of the present invention.
Indeed, it is appreciated that the specific example voltages, thicknesses, material
types, etc., are provided for explanation purposes and that other values may also
be employed in other embodiments and examples in accordance with the teachings of
the present invention.
EMBODIMENTS
[0052] Although the present invention is defined in the attached claims, it should be understood
that the present invention can also (alternatively) be defined in accordance with
the following embodiments:
- 1. A heterostructure semiconductor device comprising:
a first active layer;
a second active layer disposed on the first active layer, a two-dimensional electron
gas layer forming between the first and second active layers;
a first gate dielectric layer disposed on the second active layer;
a second gate dielectric layer disposed on the first gate dielectric layer;
a passivation layer disposed over the second gate dielectric layer;
a gate that extends through the passivation layer to the second gate dielectric layer;
first and second ohmic contacts that electrically connect to the second active layer,
the first and second ohmic contacts being laterally spaced-apart, the gate being disposed
between the first and second ohmic contacts.
- 2. The heterostructure semiconductor device of embodiment 1 wherein the second gate
dielectric layer comprises aluminum oxide (Al2O3).
- 3. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer has a first thickness and the second gate dielectric has a second
thickness, the second thickness being larger than the first thickness.
- 4. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer comprises a nitride-based compound.
- 5. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer comprises silicon nitride (SiN).
- 6. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer comprises carbon nitride (CN).
- 7. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer comprises boron nitride (BN).
- 8. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer has a first thickness in a range of about 1-5 nanometers thick.
- 9. The heterostructure semiconductor device of embodiment 1 wherein the second gate
dielectric has a second thickness in a range of about 10-20 nanometers thick.
- 10. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer has a first thickness and the second gate dielectric has a second
thickness, the first thickness and the second thickness are set such that a leakage
current through the gate is substantially constant versus temperature during normal
operation of heterojunction semiconductor device.
- 11. The heterostructure semiconductor device of embodiment 1 wherein the first gate
dielectric layer has a first thickness and the second gate dielectric has a second
thickness, the first thickness and the second thickness are set such that a threshold
voltage is substantially constant versus temperature during normal operation of heterojunction
semiconductor device.
- 12. The heterostructure semiconductor device according to embodiment 1 wherein the
first active layer comprises gallium nitride (GaN).
- 13. The heterostructure semiconductor device of embodiment 1 wherein the second active
layer comprises aluminum gallium nitride (AlGaN).
- 14. The heterostructure semiconductor device of embodiment 1 wherein the first and
second active layers are defined as an isolated mesa.
- 15. The heterostructure semiconductor device of embodiment 1 wherein the gate comprises
a gate metal.
- 16. The heterostructure semiconductor device of embodiment 15 wherein the gate metal
comprises a nickel gold (NiAu) alloy.
- 17. The heterostructure semiconductor device of embodiment 15 wherein the gate metal
includes a gate field plate that extends toward the drain ohmic contact.
- 18. The heterostructure semiconductor device of embodiment 1 wherein the passivation
layer comprises silicon nitride (SiN).
- 19. The heterostructure semiconductor device of embodiment 1 wherein the gate metal
comprises titanium gold (TiAu) alloy or molybdenum gold MoAu alloy.
- 20. A method of fabricating a heterostructure semiconductor device comprising:
forming a first active layer on a substrate;
forming a second active layer on the first active layer, the first active layer and
the second active layer having different bandgaps such that a two-dimensional electron
gas layer is formed therebetween;
forming a first gate dielectric layer on the second active layer, the first gate dielectric
layer having a first thickness;
forming a second gate dielectric layer on the first gate dielectric layer, the second
gate dielectric layer having a second thickness greater than the first thickness;
forming first and second ohmic contacts that each extend vertically through the second
gate dielectric layer, and the first gate dielectric layer, the first and second ohmic
contacts being laterally spaced-apart and electrically connected to the second active
layer; and
forming a gate that contacts the second dielectric layer at a lateral position between
the first and second ohmic contacts.
- 21. The method of embodiment 20 further comprising depositing, prior to the forming
of the first and second ohmic contacts, a passivation layer over the second gate dielectric
layer.
- 22. The method of embodiment 20 further comprising annealing the second gate dielectric
layer.
- 23. The method of embodiment 20 further comprising annealing the first and second
ohmic contacts.
- 24. The method of embodiment 20 wherein the first thickness and the second thickness
are selected such that a gate leakage current remains substantially constant over
temperature during a normal operation of the heterostructure semiconductor device.
- 25. The method of embodiment 20 wherein the first gate dielectric layer comprises
silicon nitride.
- 26. The method of embodiment 20 wherein the second gate dielectric layer comprises
aluminum oxide.
- 27. The method of embodiment 20 wherein the first active layer comprises gallium nitride.
- 28. The method of embodiment 20 wherein the second active layer comprises aluminum
gallium nitride.
- 29. The method of embodiment 20 wherein the first gate dielectric layer is formed
in-situ with the first and second active layers.
- 30. The method of embodiment 20 wherein the first gate dielectric layer is formed
ex-situ with the first and second active layers.
- 31. The method of embodiment 20 wherein the first thickness is in a range of about
1-5 nanometers thick.
- 32. The method of embodiment 20 wherein the second thickness is in a range of about
10-20 nanometers thick.
- 33. The method of embodiment 20 wherein the forming of the second gate dielectric
layer is performed using an Atomic Layer Deposition (ALD) reaction chamber with an
Al(CH3)3 precursor and O2 plasma.
- 34. The method of embodiment 20 wherein the forming of the first and second ohmic
contacts comprises depositing a metal which includes gold (Au).
- 35. The method of embodiment 34 wherein the metal comprises TiAlMoAu.
1. A heterostructure semiconductor device comprising:
a first active layer;
a second active layer disposed on the first active layer, a two-dimensional electron
gas layer forming between the first and second active layers;
a first gate dielectric layer disposed on the second active layer;
a second gate dielectric layer disposed on the first gate dielectric layer;
a passivation layer disposed over the second gate dielectric layer;
a gate that extends through the passivation layer to the second gate dielectric layer;
first and second ohmic contacts that electrically connect to the second active layer,
the first and second ohmic contacts being laterally spaced-apart, the gate being disposed
between the first and second ohmic contacts.
2. The heterostructure semiconductor device of claim 1 wherein the second gate dielectric
layer comprises aluminum oxide (Al2O3).
3. The heterostructure semiconductor device of claim 1 or 2 wherein the first gate dielectric
layer has a first thickness and the second gate dielectric has a second thickness,
the second thickness being larger than the first thickness.
4. The heterostructure semiconductor device of any of claims 1 to 3 wherein the first
gate dielectric layer comprises a nitride-based compound, preferably silicon nitride
(SiN), carbon nitride (CN) or boron nitride (BN).
5. The heterostructure semiconductor device of anyone of claims 1 to 4 wherein the first
gate dielectric layer has a first thickness in a range of about 1-5 nanometers thick
and wherein the second gate dielectric has a second thickness in a range of about
10-20 nanometers thick.
6. The heterostructure semiconductor device of any of the preceding claims wherein the
first gate dielectric layer has a first thickness and the second gate dielectric has
a second thickness, the first thickness and the second thickness are set such that
a leakage current through the gate is substantially constant versus temperature during
normal operation of heterojunction semiconductor device or such that a threshold voltage
is substantially constant versus temperature during normal operation of heterojunction
semiconductor device.
7. The heterostructure semiconductor device according to any of the preceding claims
wherein the first active layer comprises gallium nitride (GaN) and wherein the second
active layer comprises aluminum gallium nitride (AlGaN).
8. The heterostructure semiconductor device of any of the preceding claims wherein the
first and second active layers are defined as an isolated mesa.
9. The heterostructure semiconductor device of any of the preceding claims wherein the
gate comprises
a nickel gold (NiAu) alloy, titanium gold (TiAu) alloy or molybdenum gold MoAu alloy,
preferably wherein the gate metal includes a gate field plate that extends toward
the drain ohmic contact.
10. The heterostructure semiconductor device of any of the preceding claims wherein the
passivation layer comprises silicon nitride (SiN).
11. A method of fabricating a heterostructure semiconductor device comprising:
forming a first active layer on a substrate;
forming a second active layer on the first active layer, the first active layer and
the second active layer having different bandgaps such that a two-dimensional electron
gas layer is formed therebetween;
forming a first gate dielectric layer on the second active layer, the first gate dielectric
layer having a first thickness;
forming a second gate dielectric layer on the first gate dielectric layer, the second
gate dielectric layer having a second thickness greater than the first thickness;
forming first and second ohmic contacts that each extend vertically through the second
gate dielectric layer, and the first gate dielectric layer, the first and second ohmic
contacts being laterally spaced-apart and electrically connected to the second active
layer; and
forming a gate that contacts the second dielectric layer at a lateral position between
the first and second ohmic contacts.
12. The method of claim 11 further comprising depositing, prior to the forming of the
first and second ohmic contacts, a passivation layer over the second gate dielectric
layer.
13. The method of claim 11 or 12 further comprising:
annealing the second gate dielectric layer; and
annealing the first and second ohmic contacts.
14. The method of anyone of claims 11 to 13 wherein the first gate dielectric layer is
formed in-situ with the first and second active layers or wherein the first gate dielectric
layer is formed ex-situ with the first and second active layers.
15. The method of anyone of claims 11 to 14 wherein the forming of the second gate dielectric
layer is performed using an Atomic Layer Deposition (ALD) reaction chamber with an
Al(CH3)3 precursor and O2 plasma.